Work-Energy problem involving pulley

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    Pulley Work-energy
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Homework Help Overview

The discussion revolves around a work-energy problem involving a pulley system with two blocks, where a constant force is applied to one block while the other block's motion is dependent on the first. Participants are tasked with determining the velocity of block B after block A moves a certain distance and the tension in the cable, while neglecting the masses of the pulleys and friction.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss different methods to analyze the system, including treating the blocks as a single system versus separate systems. There are attempts to derive equations for forces and accelerations based on free body diagrams. Some participants question the validity of their calculations and the assumptions made regarding the relationships between the blocks' motions.

Discussion Status

The discussion is ongoing, with participants sharing their calculations and results. Some have expressed uncertainty about their findings, while others have provided feedback on the equations used. There is a mix of interpretations regarding the setup and the relationships between the blocks, indicating a productive exploration of the problem.

Contextual Notes

Participants note potential errors in their calculations and the importance of correctly applying the equations of motion. There is also mention of the need to clarify the roles of tension and weight in the system, as well as the implications of using different coordinate systems for analyzing the motion.

thepatient
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Homework Statement


The system shown is at rest when a constant 250N force is applied to block A. Neglecting masses of pulleys and friction, determine:
a) Velocity of block B after block A moved 2 m.
b) The tension in the cable
http://imageshack.us/photo/my-images/259/photoivl.jpg/

Homework Equations



Fnet = ma.

U = mgh

KE = 1/2 mv^2

Ui + KEi + W = Uf + KEf, where subindex i and f mean initial and final states.

The Attempt at a Solution



I have completed this problem, but I'm not sure if this is correct. The professor said this particular problem can be done by taking both masses and the ropes as a single system and also by taking each mass as its own, separate system. I did took each as a separate system.

First, I drew a free body diagram for block A. The net force in the x direction, assuming left is negative gives me:

F - T = ma_A
1------------------250N - T = ma_A

The relationship between the position of block A and block B was obtained and determined to be:
X_A + 3X_B = constant. Taking first time derivative:
V_A + 3V_B = 0
V_A = - 3V_B. Second time derivative:
2--------------a_A = -3a_B

Using Newton's law for the y direction on block B:
up positive: 3T - W = m*a_B
3-----------3T - mg = m*a_B

Solving 1 for acceleration a_A, then using equation 2 to leave as a_B = form:
250-T/m_a = -3a_B
4----- -250+T/(3m_a) = a_B

Using 4 to solve for tension in 3:
3T - m_b*g = -m_b*250/(3*m_a) + m_b * T/(3m_a)

Subsituting for values of mass of b, g, mass of a and solving for T:
T(3-25/90) = 25*9.81 - 25*250/(3*30)
T = 64.6N


Then, with that tension, using the work energy theorem on block A:

Wtension + Wconst force = 1/2 m_a V_a^2
250*2 - 129.2 = 1/2 *30va^2
V_a = 4.97 m /s <------ left.

Using relationship:
V_a = -3Vb
V_b = 1.66 m / s Upwards.





Does that seem right...? Thanks a ton. :]
 
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Both bodies move along the rope, there is no reason to distinguish between x and y components of velocity. When A moves to the left, B will move vertically upward. Taking "to the left" as positive direction for A, "up" is positive for B. You correctly figured out that the acceleration of A is three times the acceleration of B. So aA=3aB.
The equations for the accelerations and forces you wrote are correct with this choice of the direction of accelerations:

25-T=mAaA
and
3T-mBg=mBaB

Proceed from here, but do not forget the parentheses. You had at least one error by ignoring them.

ehild
 
I tried it again and more carefully this time, but used only the magnitudes of acceleration in F =ma equations. I ended up getting a tension of about 96N I think. I can try the calculation here on my phone. XD

250-T = 25a_a
3T - 30g = 30 a_b

a_A = 3a_B

Plugging 3a_B in first equation:
250 - T = 75a_B

1/75 (250 - T) = a_B =1/30(3T - 30g)
250/75 -T/75 = T/10 - g

T/75 + T/10 = 250/75 + g
T + 7.5T = 250 + 75g
Oh great now I get T = 116N :/
 
No wait I think that's what I got for my original calculation actually. And velocity of block A comes out to be 4.63 m/s to the left using the W-E theorem and the speed of block B a third of that value.
 
thepatient said:
I tried it again and more carefully this time, but used only the magnitudes of acceleration in F =ma equations. I ended up getting a tension of about 96N I think. I can try the calculation here on my phone. XD

250-T = 25a_a
3T - 30g = 30 a_b

The masses are interchanged in the equations above: ma = 30 kg and mb=25 kg. Your first calculation was correct, T=95.9 N.
 
thepatient said:
No wait I think that's what I got for my original calculation actually. And velocity of block A comes out to be 4.63 m/s to the left using the W-E theorem and the speed of block B a third of that value.


I got va=4.63 m/s, vb=1.51 m/s, but it seems all right otherwise.

ehild
 
Thanks a ton. :]
 
You are welcome. It was a nice solution of a nice problem:smile:


ehild
 
thepatient can you explain how you arrived at 3T-W=mbab ?
 
  • #11
  • #12
It is the weight downwards and three times the tension in the string upwards, as the block is held by three threads of the string.
What do you mean on "the normal of its weight"?

ehild
 
  • #13
Uh sorry my bad, I was referring to the normal reaction on an object kept on a table lol xD here it doesn't apply sorry
 

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